The \(\langle KE_{T} \rangle \)  for \({K_{s}}^{0}\) , \(\Lambda \)  and \(\Xi \)  particles as a function of multiplicity are shown in Figure REF .
For all particle species, \(\langle KE_{T} \rangle \)  increases with increasing multiplicity. A theoritical Blast-wave model [1]} fits have also been performed to the \(p_{\rm T}\)  spectra of strange particles
in several multiplicity bins as shown in Figure REF . The interpretation of the parameters of these fits, such as kinetic freeze-out temperature, \(T_{kin}\)  and
transverse radial flow velocity, \(\beta _{T}\) , are model dependent.
In the context of the Blast-Wave model, when comparing the parameters of different systems at similar \(dN_{ch}/d\eta \) ,
it was found that \(\beta _{T} \)  is larger for small systems i.e., \(\beta _{T} {\rm (pp)} >\)  \(\beta _{T} {\rm (pPb)} >\)  \(\beta _{T}{\rm (PbPb)} \) .
This could be an indication of a larger radial flow in small systems as a consequence of stronger pressure gradients due to a more explosive system.
However, a similar decreasing trend is observed for \(T_{kin}\)  and \(\beta _{T}\)  as a function of multiplicity in all three collision systems.
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